Practical Guige to Free Energy Devices

The results indicate that the highest mass-bound power assembled by the secondary transmitter circuit does not
exceed 7 watts - and this is directly output from the secondary 26 when the load is 50 Megohm, or from the
transmitter plate when the load is 1 Megohm. The mass-bound electric power emulated by the receiving circuit
(plate, coil and Function Y without the plasma pulser circuitry) never exceeds the mass-bound electric power
outputted directly by the transmitter, and peaks when the resistive load value (1 Megohm) approaches the prebreakdown
resistance range of the vacuum tube, at 4.72W. These findings then indicate that when the
transmitter circuit is consuming a maximum of 35W, a typical output from the secondary of the transmitter is 7W,
and at 3'' of distance within the proximal field of the latter, the pick-up by a tuned receiver will be of the order of
5W of mass-bound current duplicated within the receiving coil. The loss in the first stage is therefore on the order
of sevenfold.
Continuing with the description of the circuit of Fig.19, a 128 cm 2 plate area, 6 cm gap PAGD reactor is used,
connected as described in our prior art to a high-vacuum rotary pump (Correa, P & Correa, A (1995) "Energy
conversion system", U.S. Pat. No. 5,449,989). Pressure readings were obtained with a thermocouple gauge
during the operational runs. The KS-9303 motors to be tested are then connected to the PAGD reactor in the
usual capacitatively-coupled, inverter fashion described in our prior art (Correa, P & Correa, A (1995)
"Electromechanical transduction of plasma pulses", U.S. Pat. No 5,416.391). Their rpm is detected by a
stroboscopic tachometer and fed to a Mac Performa 6400 running a motor algorithm program calculating the
power output. Motor measurements were made at five minutes into each run for the unloaded motors, and at ten
minutes for the inertially dampened motors.
All experiments were carried out in the same work session. The experimental determination of the continuous
rotary power output as a function of the reactor pulse rate confirmed that the improved circuit develops maximum
rotary capture of the mass-free energy in the receiver circuit at the lowest rates of pulsation, just as we have
previously found for the conversion system of U.S. Pat. No. 5,449,989. Furthermore, the data showed that even
motors of type KS-8624 are able to output power mechanically in excess of the mass-bound power output by the
transmitter (7W) or captured by the receiver (5 to a max. of 7W), once the PAGD rate decreases to 1.5 PPS.
Such an anomaly can only be explained by the system having become able to begin capturing the mass-free
energy flux in the receiver circuit that we know already is output by the transmitter circuit. But this excess
mechanical power is still less than the power input into the transmitter, and clearly so. It represents a power gain
with respect to the secondary, but a loss with respect to the primary. The full breadth of the capture of the massfree
electric energy flux circulating in the receiver circuit is not seen until the motors are resonantly loaded
because they are inertially dampened.
The KS-9303 motors, once inertially dampened, and thus loaded, are able to recover enough power from the
mass-free energy field to develop a mechanical power, not just greatly in excess of the mass-bound power of the
secondary, but also greatly in excess of the mass-bound power input to the vibrator stage and the primary, at 28
to 35W. Once the pulse rate approaches the same 1.5 PPS marker, mechanical power in excess of the massbound
electric power input to the primary becomes evident, peaking at nearly three times that input. In fact, the
highest output recorded was also obtained with the lowest input to the transmitter circuit, the highest exact
coefficient observed in this experiment being 100.8W / 28W = 3.6. Furthermore, with respect to the secondary
mass-bound output, the same mechanical rotary output represents a much greater overunity coefficient of
performance, on the order of 14.4 times greater. This is at least partly the result of the receiver and motor capture
of the mass-free electric energy output by the transmitter, and may be partly the result of mass-free energy
engrafted by the PAGD regime in the PAGD reactor.
Reviewing the mechanical power output results as a function of increasing vacuum in the PAGD reactor and at
different output power levels, any motor performance below the 5-7W limit of the traditional mass-bound output
power of the secondary represents an output mechanical power loss with respect to both the mass-bound
secondary output and the mass-bound primary input. All the results for pressures down to 0.03 Torr fall into this
category, and thus represent a very inefficient coupling to the PAGD regime. Any motor performance between
7W and 28-35W represent a loss with respect to the electrical power input to the transmitter system, but a net
gain of power with respect to the mass-bound secondary power output. None of the non-inertially dampened
motors tested were able to perform outside of this area, under the test conditions. With more efficient primary to
secondary couplings in the transmitter station, however, one could advantageously employ these motors alone to
extract some of the mass-free power of the secondary or to operate them in enclosed vessels without
conventional external electrical connections.
To reach satisfactory levels of recovery of mass-free energy, one must dampen the superimposed DW impulses.
Hence, all results showing outputs in excess of 35W were obtained using the inertially dampened KS-9303
motors, and represent a net overunity power gain over both the power input to the primary and the mass-bound
power output by the secondary, or the mass-bound power emulated by the receiver circuitry. This happens when
the PAGD pulse rate falls to 2 PPS, with the rotary power output steeply increasing as the rate falls to 1 PPS.
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